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roseta

Last edited: August 8, 2025

Rosetta

Last edited: August 8, 2025

Rosetta is a set of physical-based protein folding models.

protein binding with Rosetta

  • check a protein surface
  • check how protein side-chains interact with the binding surface

peptide binding with Rosetta

The difficulty with this is that we don’t know what the overall tertiary structure of a group of peptides are; unlike whole protein binding.

sequence-specific DNA binding

???

more!

You take something like a trimer; you shove a peptide between each “point”, and boom structal change to a quadromer

RoseTTAFold2

Last edited: August 8, 2025

RoseTTAFold2 is a three-track folding tool, which also handles multimer!

  1. inputs: amino acid sequence + CHEMICAL structure (WOAH! how?)
  2. “RF2 all-atom embedding”
  3. fold!

The model does really well!

application: de-novo luciferase design

  1. come up with the correct shaped scaffolds
  2. use old Rosetta to jam a residue sequence into the scaffold
  3. refold

application: RoseTTAFold2 in-painting

Train the model to recover the missing bits of sequence from the overall structure (i.e. training backwards), and

Rossing 1990

Last edited: August 8, 2025

On the dynamics of Tuning Forks. (Rossing, Russell, and Brown 1992)

Characterizing Tuning Forks

Aluminum, tines 10mm apart. Four main groups of vibration:

  1. Symmetrical In-Plane
  2. Antisymmetrical In-Plane
  3. Symmetrical Out-Of-Plane
  4. Antisymmetrical Out-Of-Plane

(a) and (c) are in the first group; (b) is in the second group, where the fork just warps.

Deriving Tuning Forks’ Frequency

As per before, we can treat tuning forks acting in clang and fundamental modes as a good’ol fashioned cantilever beam.

rotational energy theorem

Last edited: August 8, 2025

total kinetic energy

\begin{equation} KE_{rigid} = \frac{1}{2} M{V_{cm}}^2 + \frac{1}{2} I_{CM}{\omega_{CM}}^2 \end{equation}

torque from gravity

For even non rigid bodies, the following follows:

\begin{equation} \vec{\tau}_g = \vec{R}_{CM} \times M\vec{g} \end{equation}

Actually, this follows for any \(f\) (like \(g\)) evenly applied across point masses.

potential energy

\begin{equation} \Delta PE_g = mg\Delta h \end{equation}

where, \(\Delta h\) is the travel of center of mass. Regardless of whether or not its point.